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3-Forms, Axions and D-Brane Instantons

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3-Forms, Axions and D-Brane Instantons 3-Forms, Axions and D-brane Instantons Eduardo Garc´ıa-Valdecasas Tenreiro Instituto de F´ısica Teorica´ UAM/CSIC, Madrid Based on 1605.08092 by E.G. & A. Uranga V Postgradute Meeting on Theoretical Physics, Oviedo, 18th November 2016 Axions, Monodromy and 3-Forms String Theory, D-Branes and Instantons Backreacting Instantons Motivation & Outline Motivation Axions have very flat potentials ) Good for Inflation. Axions with non-perturbative (instantons) potential can always be described as a 3-Form eating up the 2-Form dual to the axion. There is no candidate 3-Form for stringy instantons. We will look for it in the geometry deformed by the instanton. Outline 1 Axions, Monodromy and 3-Forms. 2 String Theory, D-Branes and Instantons. 3 Backreacting Instantons. Eduardo Garc´ıa-Valdecasas Tenreiro 3-Forms, Axions and D-brane Instantons 2 / 20 2 / 20 Axions, Monodromy and 3-Forms String Theory, D-Branes and Instantons Backreacting Instantons Axions and Monodromy. Axions are periodic scalar fields. This shift symmetry can be broken to a discrete symmetry by non-perturbative effects ! Very flat potential, good for inflation. The discrete shift symmetry gives periodic potentials, but non-periodic ones can be used by endowing them with a monodromy structure. For instance: jφj2 + µ2φ2 (1) Superplanckian field excursions in Quantum Gravity are under pressure due to the Weak Gravity Conjecture (Arkani-Hamed et al., 2007). Monodromy may provide a workaround (Silverstein & Westphal, 2008; Marchesano et al., 2014). This mechanism can be easily realized in string theory. Eduardo Garc´ıa-Valdecasas Tenreiro 3-Forms, Axions and D-brane Instantons 3 / 20 3 / 20 Axions, Monodromy and 3-Forms String Theory, D-Branes and Instantons Backreacting Instantons Kaloper-Sorbo Monodromy A quadratic potential with monodromy can be described by a Kaloper-Sorbo lagrangian (Kaloper & Sorbo, 2009), 2 2 j dφj + nφF4 + jF4j (2) Where the monodromy is given by the vev of F4, different fluxes correspond to different branches of the potential. (Ibanez et al., 2016) Eduardo Garc´ıa-Valdecasas Tenreiro 3-Forms, Axions and D-brane Instantons 4 / 20 4 / 20 Axions, Monodromy and 3-Forms String Theory, D-Branes and Instantons Backreacting Instantons Kaloper-Sorbo Monodromy Monodromy structure visible in potential solving E.O.M, 2 V0 ∼ (nφ − q) ; q 2 Z (3) So there is a discrete shift symmetry, φ ! φ + φ0; q ! q + nφ0 (4) A dual description can be found using the hodge dual of φ, b2, 2 2 j db2 + nc3j + jF4j ; F4 = dc3 (5) The flatness of the axion potential is protected by gauge invariance, c3 ! c3 + dΛ2 ; b2 ! b2 − nΛ2 (6) We will look for a three form c3 coupling to the axion as ∼ φF4 This description has the periodicity built in. Whenever the potential breaks it, there will be monodromy in the UV. Eduardo Garc´ıa-Valdecasas Tenreiro 3-Forms, Axions and D-brane Instantons 5 / 20 5 / 20 Axions, Monodromy and 3-Forms String Theory, D-Branes and Instantons Backreacting Instantons Example: Peccei-Quinn mechanism in 3-Form language. Strong CP problem: QCD has an anomalous U(1)A symmetry producing a physical θ-term. g2θ L ∼ F a F~ aµν (7) 32π2 µν Where θ classifies topologically inequivalent vacua and is typically ∼ 1. This term breaks CP and experimental data −10 constrain θ . 10 ! Fine Tuning. Solution: PQ Mechanism. New anomalous spontaneously broken U(1)PQ. So θ is promoted to pseudo-Goldstone boson, the axion. Non-perturbative effects give it a potential and fix θ = 0. Eduardo Garc´ıa-Valdecasas Tenreiro 3-Forms, Axions and D-brane Instantons 6 / 20 6 / 20 Axions, Monodromy and 3-Forms String Theory, D-Branes and Instantons Backreacting Instantons Example: Peccei-Quinn mechanism in 3-Form language. The term can be rewritten as (Dvali, 2005), g2 3 θFF~ ∼ θF = θ dC ; C = Tr A A A − A @ A 4 3 αβγ 8π2 [α β γ] 2 [α β γ] (8) So, making θ small = How can I make the F4 electric field small? Solution: Screen a field ) Higgs mechanism. Let C3 eat a 2-Form b2! ) b2 is Hodge dual of axion! Potential for the axion () 3-Form eating up a 2-form. Eduardo Garc´ıa-Valdecasas Tenreiro 3-Forms, Axions and D-brane Instantons 7 / 20 7 / 20 Axions, Monodromy and 3-Forms String Theory, D-Branes and Instantons Backreacting Instantons String Theory String theory unifies gravity and quantum mechanics. String theory aims to describe everything as vibrations of tiny strings (see IFT youtube). ! Each particle is a different vibration state of the string ) So string theory is awesome! Caveats: 10 dimensions, infinite (or very big) landscape of vacua, only pertubatively defined... But who cares? ! Gravity is described by closed strings and gauge interactions by open strings. ! 6 dimensions are compact: M4 × X 6 Eduardo Garc´ıa-Valdecasas Tenreiro 3-Forms, Axions and D-brane Instantons 8 / 20 8 / 20 Axions, Monodromy and 3-Forms String Theory, D-Branes and Instantons Backreacting Instantons D-Branes Open Strings end on non-perturbative, dynamical objects called D-Branes, ! Rich physcis inside the Brane. Eduardo Garc´ıa-Valdecasas Tenreiro 3-Forms, Axions and D-brane Instantons 9 / 20 9 / 20 Axions, Monodromy and 3-Forms String Theory, D-Branes and Instantons Backreacting Instantons D-Brane Instantons Dp-Branes completely wrapped around euclidean p cycles are D-brane instantons. There are two kinds: Dp-Brane instanton inside D(p + 4)-Brane ! Gauge Instanton. Dp-Brane alone ! Stringy Instanton. ) We study non-perturbative potentials for axions coupling to stringy instantons. There are 5 string theories, all related through dualities. We will focus on type IIB. It has odd Dp-branes and odd RR Forms: F1; F3; F5::: Eduardo Garc´ıa-Valdecasas Tenreiro 3-Forms, Axions and D-brane Instantons 10 / 20 10 / 20 Axions, Monodromy and 3-Forms String Theory, D-Branes and Instantons Backreacting Instantons Axions in String Theory. Axions are ubiquitous in string theory. For instance upon compactification, Z a(x) = Cp (9) Σp Where the shift symmetry arises from the gauge invariance of the RR form. Monodromy can be realised in many ways in string theory. For instance, as unwinding of a brane (Silverstein & Westphal, 2008), Eduardo Garc´ıa-Valdecasas Tenreiro 3-Forms, Axions and D-brane Instantons 11 / 20 11 / 20 Axions, Monodromy and 3-Forms String Theory, D-Branes and Instantons Backreacting Instantons The puzzle Axion potentials come from non-perturbative effects and can be described by a 3-form eating up a 2-form. For instance, for gauge D-brane instantons it is the CS 3-Form (Dvali, 2005). For stringy instantons ! No candidate 3-Form! ) Solution: look for the 3-Form in the backreacted geometry (Koerber & Martucci, 2007). In the backreacted geometry the instanton disappears and its open-string degrees of freedom are encoded into the geometric (closed strings) degrees of freedom. Both descriptions are related in an ”holographic” way. Eduardo Garc´ıa-Valdecasas Tenreiro 3-Forms, Axions and D-brane Instantons 12 / 20 12 / 20 Axions, Monodromy and 3-Forms String Theory, D-Branes and Instantons Backreacting Instantons SU(3) × SU(3) structure manifolds. The backreacted geometry will, generically, be a non CY, SU(3) × SU(3) (1) (2) structure manifold. This structure has two globally well defined spinors η+ ; η+ , (1) (2) with c.c. η− ; η− . Define two polyforms (assume type IIB): i X 1 (2)y (1) m m Ψ± = − η γm :::m η dy l ^ ::: ^ dy 1 (10) jjη(1)jj2 l! ± 1 l + l Organize 10d fields in holomorphic polyforms, 3A−Φ −Φ Z ≡ e Ψ2; T ≡ e Re Ψ1 + i∆C (11) For an SU(3) structure manifold, η(1) ∼ η(2) and one recovers Z ∼ Ω, T ∼ eiJ Eduardo Garc´ıa-Valdecasas Tenreiro 3-Forms, Axions and D-brane Instantons 13 / 20 13 / 20 Axions, Monodromy and 3-Forms String Theory, D-Branes and Instantons Backreacting Instantons Backreacting a D3-instanton Consider type IIB String Theory with a D3-instanton wrapping a 4-cycle Σ4 in a CY3. One can show from the SUSY conditions for the D3-instanton that the backreaction is encoded in a contribution to Z (Koerber & Martucci, 2007): d(δZ) ∼ Wnpδ2(Σ4) (12) ) So, the backreaction produces a 1-form Z1 that didn’t exist in the original geometry. Note that Z1 is not closed and thus not harmonic. Eduardo Garc´ıa-Valdecasas Tenreiro 3-Forms, Axions and D-brane Instantons 14 / 20 14 / 20 Axions, Monodromy and 3-Forms String Theory, D-Branes and Instantons Backreacting Instantons The 3-form and the KS coupling Let us define α1 ≡ Z1 and β2 ≡ dα1. In type IIB string theory there is a RR 4-form C4. We may expand it as, C4 = α1(y) ^ c3(x) + β2(y) ^ b2(x) + ::: (13) ) So we have a 3-form and a 2-form dual to an scalar. We see that, F5 = dC4 = β2 ^ (c3 + db2) − α1 ^ F4 (14) Which describes a 3-Form eating up a 2-Form, as we wanted! Furthermore, Z Z Z Z F5 ^ ∗F5 = − C4 ^ dF5 ! C4 ^ β2 ^ F4 = φF4 (15) 10d 10d 10d 4d Which is the KS coupling we were looking for. Eduardo Garc´ıa-Valdecasas Tenreiro 3-Forms, Axions and D-brane Instantons 15 / 20 15 / 20 Axions, Monodromy and 3-Forms String Theory, D-Branes and Instantons Backreacting Instantons Toroidal examples. ~ For a 4-cycle defined by the equation f = 0 the 1-form is Z(1) ∼ df Wnp. Example 1: Factorisable 6-torus, M4 × T2 × T2 × T2 with local coordinates z1; z2; z3 and take the cycle f = z3 = 0, −T Z(1) ∼ e dz3 (16) ) already in the original geometry, because T6 is non-CY.
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